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Delft University of Technology Wind turbine rotor aerodynamics The IEA MEXICO rotor explained PDF

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Delft University of Technology Wind turbine rotor aerodynamics The IEA MEXICO rotor explained Zhang, Ye DOI 10.4233/uuid:f8112b0f-d697-4e5c-bbff-ea7eae5ab50c Publication date 2017 Document Version Final published version Citation (APA) Zhang, Y. (2017). Wind turbine rotor aerodynamics: The IEA MEXICO rotor explained. https://doi.org/10.4233/uuid:f8112b0f-d697-4e5c-bbff-ea7eae5ab50c Important note To cite this publication, please use the final published version (if applicable). Please check the document version above. Copyright Other than for strictly personal use, it is not permitted to download, forward or distribute the text or part of it, without the consent of the author(s) and/or copyright holder(s), unless the work is under an open content license such as Creative Commons. Takedown policy Please contact us and provide details if you believe this document breaches copyrights. We will remove access to the work immediately and investigate your claim. This work is downloaded from Delft University of Technology. For technical reasons the number of authors shown on this cover page is limited to a maximum of 10. (cid:105) (cid:105) “dissertation” — 2017/6/18 — 23:43 — page i — #1 (cid:105) (cid:105) WIND TURBINE ROTOR AERODYNAMICS THE IEA MEXICO ROTOR EXPLAINED (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) “dissertation” — 2017/6/18 — 23:43 — page ii — #2 (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) “dissertation” — 2017/6/18 — 23:43 — page iii — #3 (cid:105) (cid:105) WIND TURBINE ROTOR AERODYNAMICS THE IEA MEXICO ROTOR EXPLAINED Proefschrift terverkrijgingvandegraadvandoctor aandeTechnischeUniversiteitDelft, opgezagvandeRectorMagnificusprof.ir.K.C.A.M.Luyben, voorzittervanhetCollegevoorPromoties, inhetopenbaarteverdedigenopwoensdag14juni2017om12:30uur door YE ZHANG MasterofScienceinThermalEnergyandPowerEngineering DalianUniversityofTechnology,Dalian,China geborenteHeilongjiang,China. (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) “dissertation” — 2017/6/18 — 23:43 — page iv — #4 (cid:105) (cid:105) Thisdissertationhasbeenapprovedby: promotor:Prof.dr.ir.G.J.W.van Bussel copromotor:Dr.ir.A.H.vanZuijlen Compositionofthedoctoralcommittee: RectorMagnificus, voorzitter Prof.dr.ir.G.J.W.van Bussel TechnischeUniversiteitDelft,promotor Dr.ir.A.H.vanZuijlen TechnischeUniversiteitDelft,copromotor Independentmembers: Prof.dr.ir.G.Eitelberg TechnischeUniversiteitDelft Prof.dr.N.N.Sørensen TechnicalUniversityofDenmark Prof.dr.A.P.Schaffarczyk KieUniversity,Germany Dr.ir.J.G. Schepers EnergyresearchCentreoftheNetherlands Othermembers: Prof.dr.ir.drs H.Bijl TechnischeUniversiteitDelft&Leiden Reservedmembers: Prof.dr.ir.G.A.M.vanKuik TechnischeUniversiteitDelft (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) “dissertation” — 2017/6/18 — 23:43 — page v — #5 (cid:105) (cid:105) v Keywords: MEXICOrotor,rotoraerodynamics,CFD,OpenFOAM,ZigZageffects, loads overprediction, transition modeling, turbulence modeling, de- tachededdysimulation,PIV Printedby: ProefschriftMaken Cover: Photo is taken from https://www.evwind.es/2015/07/04/offshore- wind-power-630-mw-london-array-wind-farm-with-175-wind- turbines/53165 Copyright©2017byYeZhang ISBN978-94-6186-815-2 Anelectronicversionofthisdissertationisavailableat http://repository.tudelft.nl/. (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) “dissertation” — 2017/6/18 — 23:43 — page vi — #6 (cid:105) (cid:105) Tomyfamily,fortheirpatience,supportandlove (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) “dissertation” — 2017/6/18 — 23:43 — page vii — #7 (cid:105) (cid:105) C ONTENTS Summary ix Samenvatting xi 1 Introduction 13 1.1 Researchbackground. . . . . . . . . . . . . . . . . . . . . . . . . . . . 14 1.2 Motivationandobjectives. . . . . . . . . . . . . . . . . . . . . . . . . . 19 1.3 Thesisoutline. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 21 2 Windturbineaerodynamics 23 2.1 2Dairfoilaerodynamics. . . . . . . . . . . . . . . . . . . . . . . . . . . 24 2.2 3Dfinitewingaerodynamics . . . . . . . . . . . . . . . . . . . . . . . . 26 2.3 Windturbinebladeaerodynamics . . . . . . . . . . . . . . . . . . . . . 29 2.4 Rotoraerodynamicsmodeling . . . . . . . . . . . . . . . . . . . . . . . 30 2.4.1 Bladeelementmomentummethod . . . . . . . . . . . . . . . . . 30 2.4.2 Vortexwakemodel. . . . . . . . . . . . . . . . . . . . . . . . . . 35 2.4.3 Navier-Stokesbasedmethod. . . . . . . . . . . . . . . . . . . . . 37 2.5 Conclusions. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 40 3 VerificationandvalidationofOpenFOAMcode 43 3.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 44 3.2 Validationofturbulencemodels . . . . . . . . . . . . . . . . . . . . . . 44 3.2.1 Eddyviscosityturbulencemodel. . . . . . . . . . . . . . . . . . . 44 3.2.2 HybridRANS/LESmodel. . . . . . . . . . . . . . . . . . . . . . . 51 3.3 Validationoftransitionmodels . . . . . . . . . . . . . . . . . . . . . . . 58 3.3.1 Thestructureofk−k −ωtransitionmodel . . . . . . . . . . . . . 58 L 3.3.2 k−k −ωimplementationandcorrectionsinOpenFOAM. . . . . . 58 L 3.3.3 Testcases . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 59 3.4 Conclusions. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 68 4 Experimentalandnumericalstudyofthenon-rotatingMEXICOblade 69 4.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 70 4.2 Experimentalandnumericalsetup . . . . . . . . . . . . . . . . . . . . . 70 4.2.1 Experimentalapproach . . . . . . . . . . . . . . . . . . . . . . . 70 4.2.2 Numericalapproach. . . . . . . . . . . . . . . . . . . . . . . . . 76 4.3 Resultsandanalysis. . . . . . . . . . . . . . . . . . . . . . . . . . . . . 78 4.3.1 Flowatlowanglesofattack . . . . . . . . . . . . . . . . . . . . . 78 4.3.2 TheeffectsofZigZagtape . . . . . . . . . . . . . . . . . . . . . . 90 4.3.3 Flowathighanglesofattack. . . . . . . . . . . . . . . . . . . . . 98 4.4 Conclusions. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 101 vii (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) “dissertation” — 2017/6/18 — 23:43 — page viii — #8 (cid:105) (cid:105) viii CONTENTS 5 Numericalinvestigationof3DrotatingMEXICOrotor 103 5.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 104 5.2 Windtunnelmeasurementdatabase . . . . . . . . . . . . . . . . . . . . 104 5.2.1 RotatingmeasurementsoftheMEXICOrotoratDNW. . . . . . . . 104 5.2.2 Non-rotatingmeasurementoftheMEXICObladesatTUDelft. . . . 106 5.2.3 2Dstaticairfoilwindtunnelmeasurement. . . . . . . . . . . . . . 106 5.3 RotationmodelinginOpenFOAM. . . . . . . . . . . . . . . . . . . . . . 106 5.4 Resultsanddiscussion . . . . . . . . . . . . . . . . . . . . . . . . . . . 108 5.4.1 AerodynamicloadscomparisonbetweenexperimentandBEMre- sults . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 108 5.4.2 VelocityfieldcomparisonwithPIV. . . . . . . . . . . . . . . . . . 110 5.4.3 Crosssectionalrotationaleffects . . . . . . . . . . . . . . . . . . . 114 5.4.4 RadialflowandCoriolisforce . . . . . . . . . . . . . . . . . . . . 122 5.4.5 Transitionaleffects. . . . . . . . . . . . . . . . . . . . . . . . . . 127 5.4.6 Stallconditionatλ=4.17 . . . . . . . . . . . . . . . . . . . . . . 133 5.5 Conclusions. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 137 6 AerodynamicsstudyoftheTUDelftBlade2rotor 139 6.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 140 6.2 ExperimentalandnumericaldescriptionofTUDelftBlade2rotor . . . . . 140 6.3 Resultsandanalysis. . . . . . . . . . . . . . . . . . . . . . . . . . . . . 143 6.3.1 Velocitydecomposition . . . . . . . . . . . . . . . . . . . . . . . 143 6.3.2 Forceestimationanddecomposition . . . . . . . . . . . . . . . . 148 6.4 Conclusions. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 151 7 Conclusionsandrecommendations 155 7.1 Conclusions. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 156 7.1.1 OpenFOAMperformance . . . . . . . . . . . . . . . . . . . . . . 156 7.1.2 Causesofdeviation . . . . . . . . . . . . . . . . . . . . . . . . . 157 7.1.3 Advancednumericalmodeling. . . . . . . . . . . . . . . . . . . . 158 7.2 Recommendations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 159 7.2.1 3Dfluidstructureinteraction . . . . . . . . . . . . . . . . . . . . 159 7.2.2 Flowcontrolmodelingonwindturbineblade . . . . . . . . . . . . 159 ACKNOWLEDGEMENTS 169 ListofPublications 171 CurriculumVitæ 173 (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) (cid:105) “dissertation” — 2017/6/18 — 23:43 — page ix — #9 (cid:105) (cid:105) S UMMARY Windturbinesareoperatingunderverycomplexanduncontrolledenvironmentalcon- ditions, includingatmosphericturbulence, atmosphericboundarylayereffects, direc- tional and spatial variations in wind shear, etc. Over the past decades, the size of a commercialwindturbinehasincreasedconsiderably.Allthecomplexanduncontrolled conditionsmentionedaboveresultinuncertaintiesofaerodynamicloadscalculationon verylargewindturbinebladesandthusbetternumericalcodesareneededforpredicting theloadsinthedesignphase. Withtheaimtoeliminatetheseuncontrolledeffectsand improvetheaerodynamicmodels,inlastdecades,severalimportantexperimentalcam- paignsofdifferentwindturbinemodelshavebeenperformedinlargewindtunnels.The objectiveofsuchexperiments(e.g.usingtheNRELwindturbineandtheMEXICOrotor) istoprovidehighqualitymeasurementdatawhichcanbeusedtovalidatenumerical modelsandimprovedifferentfidelitynumericalcodes,particularlyforpredictingwind turbineaerodynamicloads. Problems arose as a result of blind comparisons between (initially not disclosed) measureddataandnumericalpredictions,inwhichlargedeviationswereobservedin bothcomparisoncampaigns, evenattheeasy-to-predictconditions. Forinstance, all numerical models, including high fidelity CFD codes, show a poor prediction of sec- tionalnormalforcefortheMEXICOrotoratdesigntipspeedratio,especiallyasignifi- cantoverpredictionatthetipregion(r/R=0.82,0.92).Thesediscrepanciesareobserved andpresentedinmanyresearchreportsandpublicationswithoutaclearunderstanding ofthecauses. Therefore,inthisthesis,adetailedandthoroughinvestigationofwindturbinerotor aerodynamicsisperformedwithbothexperimentalandnumericalapproaches. Firstly, theopensourceCFDcode(OpenFOAM-2.1.1)isimprovedandvalidatedtoobtainbetter windturbineaerodynamicsloadsprediction. Beforeapplyingtheopensourcecodefor investigatingcomplex3Dflow,anOpenFOAMcodehasbeenextensivelyvalidatedand evaluatedforseveraltwo-dimensionalflowcases,whichispresentedinChapter3. The numericalresultsoftheOpenFOAMcodecomparewellwithanotheralreadyvalidate code,theoreticalsolutionorexperimentaldata. Themostpopularlineareddyviscos- ityturbulencemodels(Spalart-Allmarasandk−ωSST),implementedinOpenFOAM, havebeenvalidated. Moreover,animplementationerrorofrecentlydevelopedtransi- tionmodelk−k −ωinOpenFOAMhasbeencorrectedandthecodehasbeenfurther L improvedtopredictlaminar-turbulentboundarylayertransitiononawindturbineair- foil. Basedonthenumericalresultsofthesetwo-dimensionalcases,confidenceisob- tainedforsimulatingmorecomplex3Dflowusingthiscode. Secondly,thecausesoflargediscrepanciesbetweentheMEXICOmeasurementand the numerical results are identified in the thesis. This has been accomplished by re- assessingtheloadspredictioninthefirstMEXICOcampaignandanalyzingthepossible causesofdiscrepanciessuchas:1)theverycomplicatedgeometryoftheMEXICOrotor ix (cid:105) (cid:105) (cid:105) (cid:105)

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Wind turbine rotor aerodynamics: The IEA MEXICO rotor explained DOI: .. on the non-rotating MEXICO blade have been quantitatively analyzed from perior performance of the current CFD code to predict aerodynamic loads An alternative to advanced panel methods for wind turbine rotor
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